2020
DOI: 10.1103/physrevb.102.220402
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Weakly coupled alternating S=12 chains in the distorted honeycomb lattice compound Na2Cu2TeO6

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Cited by 19 publications
(37 citation statements)
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“…In Ref. [30], they show the excitation spectra with a gap of ∼18 meV can be described by a Hamiltonian with J 1 = 22.78(2) meV, J 2 = −8.73(4) meV, and a small but nonnegligible antiferromagnetic J 3 = 1.34(3) meV. These results place Na 2 Cu 2 TeO 6 in a unique position [30].…”
Section: Introductionmentioning
confidence: 85%
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“…In Ref. [30], they show the excitation spectra with a gap of ∼18 meV can be described by a Hamiltonian with J 1 = 22.78(2) meV, J 2 = −8.73(4) meV, and a small but nonnegligible antiferromagnetic J 3 = 1.34(3) meV. These results place Na 2 Cu 2 TeO 6 in a unique position [30].…”
Section: Introductionmentioning
confidence: 85%
“…In this case, and the bandwidth B can be approximated to be There is some anisotropy of the spin susceptibility, which may be due to the quasi-one-dimensional magnetic structure and impurity spins. Recently, a dimerized magnet Na 2 Cu 2 TeO 6 was proposed to be a quasi-one-dimensional chain system [24][25][26][27][28][29][30]. It has a monoclinic structure with the space group C2/m, and consists of alternating Cu 2 TeO 6 magnetic layers and Na nonmagnetic layers stacking along the c axis in a monoclinic way [24], similar to Na 3 Cu 2 SbO 6 (Refs.…”
Section: Introductionmentioning
confidence: 99%
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